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Cosmic Microwave Background Theory Antony Lewis CITA, University of Toronto

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Presentation on theme: "Cosmic Microwave Background Theory Antony Lewis CITA, University of Toronto"— Presentation transcript:

1 Cosmic Microwave Background Theory Antony Lewis CITA, University of Toronto

2 Outline Introduction and basic physics CMB temperature power spectrum and observables Parameter estimation Primordial perturbations CMB Polarization: E and B modes CMB lensing Second order effects except lensing: SZ effect (clusters), OV, etc. Mathematical details CMB data analysis etc.. Not covered

3 Source: NASA/WMAP Science Team Observations Theory

4 Hu & White, Sci. Am., 290 44 (2004) Evolution of the universe Opaque Transparent

5 Black body spectrum observed by COBE - close to thermal equilibrium: temperature today of 2.726K ( ~ 3000K at z ~ 1000 because ν ~ (1+z)) Residuals Mather et al 1994

6 Source: NASA/WMAP Science Team O(10 -5 ) perturbations (+galaxy) Dipole (local motion) (almost) uniform 2.726K blackbody Observations: the microwave sky today

7 Can we predict the primordial perturbations? Maybe.. Quantum Mechanics waves in a box calculation vacuum state, etc… Inflation make >10 30 times bigger After inflation Huge size, amplitude ~ 10 -5

8 Perturbation evolution – what we actually observe CMB monopole source till 380 000 yrs (last scattering), linear in conformal time scale invariant primordial adiabatic scalar spectrum photon/baryon plasma + dark matter, neutrinos Characteristic scales: sound wave travel distance; diffusion damping length

9 Observed ΔT as function of angle on the sky

10 Perturbations O(10 -5 ) Simple linearized equations are very accurate (except small scales) Can use real or Fourier space Fourier modes evolve independently: simple to calculate accurately Calculation of theoretical perturbation evolution Thomson scattering (non-relativistic electron-photon scattering) - tightly coupled before recombination: tight-coupling approximation (baryons follow electrons because of very strong e-m coupling) Background recombination physics (Saha/full multi-level calculation) Linearized General Relativity Boltzmann equation (how angular distribution function evolves with scattering) Physics Ingredients

11 CMB power spectrum C l Theory: Linear physics + Gaussian primordial fluctuations Theory prediction - variance (average over all possible sky realizations) - statistical isotropy implies independent of m ClCl CMBFAST: CAMB: CMBEASY: COSMICS, Initial conditions + cosmological parameters linearized GR + Boltzmann equations

12 Sources of CMB anisotropy Sachs Wolfe: Potential wells at last scattering cause redshifting as photons climb out Photon density perturbations: Over-densities of photons look hotter Doppler: Velocity of photon/baryons at last scattering gives Doppler shift Integrated Sachs Wolfe: Evolution of potential along photon line of sight: net red- or blue-shift as photon climbs in an out of varying potential wells Others: Photon quadupole/polarization at last scattering, second-order effects, etc.

13 Hu & White, Sci. Am., 290 44 (2004) CMB temperature power spectrum Primordial perturbations + later physics diffusion damping acoustic oscillations primordial power spectrum finite thickness

14 Why C l oscillations? Think in k-space: modes of different size Co-moving Poisson equation: (k/a) 2 Ф = κ δρ / 2 - potentials approx constant on super-horizon scales - radiation domination ρ ~ 1/a 4 δρ/ρ ~ k 2 a 2 Ф since Ф ~ constant, super-horizon density perturbations grow ~ a 2 After entering horizon pressure important: perturbation growth slows, then bounces back series of acoustic oscillations (sound speed ~ c/3) CMB anisotropy (mostly) from a surface at fixed redshift: phase of oscillation at time of last scattering depends on time since entering the horizon k-dependent oscillation amplitude in the observed CMB

15 Challinor: astro-ph/0403344

16 Contributions to temperature C l Challinor: astro-ph/0403344 + other

17 Anisotropy observations Current WMAP + other CMB data Redhead et al: astro-ph/0402359

18 What can we learn from the CMB? Initial conditions What types of perturbations, power spectra, distribution function (Gaussian?); => learn about inflation or alternatives. (distribution of ΔT; power as function of scale; polarization and correlation) What and how much stuff Matter densities (Ω b, Ω cdm ); ; neutrino mass (details of peak shapes, amount of small scale damping) Geometry and topology global curvature Ω K of universe; topology (angular size of perturbations; repeated patterns in the sky) Evolution Expansion rate as function of time; reionization - Hubble constant H 0 ; dark energy evolution w = pressure/density (angular size of perturbations; l < 50 large scale power; polarizationr) Astrophysics S-Z effect (clusters), foregrounds, etc.

19 Cosmic Variance: only one sky Cosmic Variance Use estimator for variance: - inverse gamma distribution (+ noise, sky cut, etc). WMAP low l l Cosmic variance gives fundamental limit on how much we can learn from CMB Assume a lm gaussian:

20 Parameter Estimation Can compute P( {ө} | data) = P( C l ({ө}) | c l obs ) Often want marginalized constraints. e.g. BUT: Large n integrals very hard to compute! If we instead sample from P( {ө} | data) then it is easy: Can easily learn everything we need from set of samples

21 Markov Chain Monte Carlo sampling Metropolis-Hastings algorithm Number density of samples proportional to probability density At its best scales linearly with number of parameters (as opposed to exponentially for brute integration) Now standard method for parameter estimation. Public CosmoMC code available at (Lewis, Bridle: astro-ph/0205436)

22 CMB data alone color = optical depth Samples in 6D parameter space

23 Contaldi, Hoekstra, Lewis: astro-ph/0302435 e.g. CMB+galaxy lensing +BBN prior Plot number density of samples as function of parameters Often better constraint by combining with other data

24 Thomson Scattering Polarization W Hu

25 CMB Polarization Generated during last scattering (and reionization) by Thomson scattering of anisotropic photon distribution Hu astro-ph/9706147

26 Polarization: Stokes Parameters - - QU Q -Q, U -U under 90 degree rotation Q U, U -Q under 45 degree rotation Spin-2 field Q + i U or Rank 2 trace free symmetric tensor θ sqrt(Q 2 + U 2 ) θ = ½ tan -1 U/Q

27 E and B polarization gradient modes E polarization curl modes B polarization e.g.

28 E and B harmonics Expand scalar P E and P B in spherical harmonics Expand P ab in tensor spherical harmonics Harmonics are orthogonal over the full sky: E/B decomposition is exact and lossless on the full sky Zaldarriaga, Seljak: astro-ph/9609170 Kamionkowski, Kosowsky, Stebbins: astro-ph/9611125

29 Primordial Perturbations fluid at redshift < 10 9 Photons Nearly massless neutrinos Free-streaming (no scattering) after neutrino decoupling at z ~ 10 9 Baryons + electrons tightly coupled to photons by Thomson scattering Dark Matter Assume cold. Coupled only via gravity. Dark energy probably negligible early on

30 Perturbations O(10 -5 ) Linear evolution Fourier k mode evolves independently Scalar, vector, tensor modes evolve independently Various linearly independent solutions Scalar modes: Density perturbations, potential flows Vector modes: Vortical perturbations Tensor modes: Anisotropic space distortions – gravitational waves velocities, v

31 General regular perturbation Scalar Adiabatic (observed) Matter density Cancelling matter density (unobservable) Neutrino density (contrived) Neutrino velocity (very contrived) Vector Neutrino vorticity (very contrived) Tensor Gravitational waves + irregular modes, neutrino n-pole modes, n-Tensor modes Rebhan and Schwarz: gr-qc/9403032 + other possible components, e.g. defects, magnetic fields, exotic stuff… General regular linear primordial perturbation -isocurvature-

32 Irregular (decaying) modes Generally ~ a -1, a -2 or a -1/2 E.g. decaying vector modes unobservable at late times unless ridiculously large early on Adiabatic decay ~ a -1/2 after neutrino decoupling. possibly observable if generated around or after neutrino decoupling Otherwise have to be very large (non-linear?) at early times Amendola, Finelli: astro-ph/0411273

33 CMB Polarization Signals Parity symmetric ensemble: Average over possible realizations (statistically isotropic): E polarization from scalar, vector and tensor modes B polarization only from vector and tensor modes (curl grad = 0) + non-linear scalars Power spectra contain all the useful information if the field is Gaussian

34 Scalar adiabatic mode E polarization only correlation to temperature T-E

35 General isocurvature models General mixtures currently poorly constrained Bucher et al: astro-ph/0401417

36 Primordial Gravitational Waves (tensor modes) Well motivated by some inflationary models - Amplitude measures inflaton potential at horizon crossing - distinguish models of inflation Observation would rule out other models - ekpyrotic scenario predicts exponentially small amplitude - small also in many models of inflation, esp. two field e.g. curvaton Weakly constrained from CMB temperature anisotropy Look at CMB polarization: B-mode smoking gun - cosmic variance limited to 10% - degenerate with other parameters (tilt, reionization, etc)

37 CMB polarization from primordial gravitational waves (tensors) Adiabatic E-mode Tensor B-mode Tensor E-mode Planck noise (optimistic) Weak lensing Amplitude of tensors unknown Clear signal from B modes – there are none from scalar modes Tensor B is always small compared to adiabatic E Seljak, Zaldarriaga: astro-ph/9609169

38 Reionization Ionization since z ~ 6-20 scatters CMB photons Measure optical depth with WMAP T-E correlation Temperature signal similar to tensors Quadrupole at reionization implies large scale polarization signal

39 Cosmic variance limited data – resolve structure in EE power spectrum (Weakly) constrain ionization history Weller, Lewis, Battye (in prep)Holder et al: astro-ph/0302404

40 Pogosian, Tye, Wasserman, Wyman: hep-th/0304188 Topological defects Seljak, Pen, Turok: astro-ph/9704231 10% local strings from brane inflation: lensing r=0.1 global defects: Other B-modes? Non-Gaussian signals

41 Regular vector mode: neutrino vorticity mode - logical possibility but unmotivated (contrived). Spectrum unknown. Lewis: astro-ph/0403583 Similar to gravitational wave spectrum on large scales: distinctive small scale

42 Primordial magnetic fields - not well motivated theoretically, though know magnetic fields exist - contribution from sourced gravity waves (tensors) and vorticity (vectors) e.g. Inhomogeneous field B = 3x10 -9 G, spectral index n = -2.9 Also Faraday rotation B-modes at low frequencies Kosowsky, Loeb: astro-ph/9601055, Scoccola, Harari, Mollerach: astro-ph/0405396 Lewis, astro-ph/0406096. Subramanian, Seshadri, Barrow, astro-ph/0303014 Tensor amplitude uncertain. Non-Gaussian signal. Check on galaxy/cluster evolution models. vector tensor Banerjee and Jedamzik: astro-ph/0410032

43 Inhomogeneous reionization Santon, Cooray, Haiman, Knox, Ma: astro-ph/0305471; Hu: astro-ph/9907103 Second order vectors and tensors: Mollerach, Harari, Matarrese: astro-ph/0310711 Small second order effects, e.g. non-Gaussian vectors tensors no reion E lensing reion

44 Extragalactic radio sources: Tucci et al: astro-ph/0307073 B modes potentially a good diagnostic of foreground subtraction problems or systematics Systematics and foregrounds, e.g. Galactic dust (143 and 217 GHz): Lazarian, Prunet: astro-ph/0111214

45 Partial sky E/B separation problem Pure E: Pure B: Inversion non-trivial with boundaries Likely important as reionization signal same scale as galactic cut Use set of E/B/mixed harmonics that are orthogonal and complete over the observed section of the sphere. Project onto the `pure B modes to extract B. (Nearly) pure B modes do exist Lewis, Challinor, Turok astro-ph/0106536

46 Underlying B-modesPart-sky mix with scalar E Recovered B modes map of gravity waves Separation method Observation Lewis: astro-ph/0305545

47 Weak lensing of the CMB Last scattering surface Inhomogeneous universe - photons deflected Observer

48 Lensing Potential Deflections O(10 -3 ), but coherent on degree scales important!

49 Lensing potential and deflection angles LensPix sky simulation code: Changes power spectra Makes distribution non-Gaussian

50 Lensed CMB power spectra Few % on temperature 10% on TE/EE polarization New lensed BB signal

51 Series expansion in deflection angle? Series expansion only good on large and very small scales Accurate calculation uses correlation functions: Seljak 96; Challinor, Lewis 2005

52 Lensing of CMB polarization Nearly white BB spectrum on large scales Lensing effect can be largely subtracted if only scalar modes + lensing present, but approximate and complicated (especially posterior statistics). Hirata, Seljak : astro-ph/0306354, Okamoto, Hu: astro-ph/0301031 Potential confusion with tensor modes Lewis, Challinor review in prep

53 Planck (2007+) parameter constraint simulation (neglect non-Gaussianity of lensed field; BB noise dominated so no effect on parameters) Important effect, but using lensed CMB power spectrum gets right answer Lewis 2005

54 Other non-linear effects Thermal Sunyaev-Zeldovich Inverse Compton scattering from hot gas: frequency dependent signal Kinetic Sunyaev-Zeldovich (kSZ) Doppler from bulk motion of clusters; patchy reionization; (almost) frequency independent signal Ostriker-Vishniac (OV) same as kSZ but for early linear bulk motion Rees-Sciama Integrated Sachs-Wolfe from evolving non-linear potentials: frequency independent General second order includes all of the above + more

55 Conclusions CMB contains lots of useful information! - primordial perturbations + well understood physics (cosmological parameters) Precision cosmology - constrain many cosmological parameters + primordial perturbations Currently no evidence for any deviations from standard near scale-invariant purely adiabatic primordial spectrum E-polarization and T-E measure optical depth, constrain reionization; constrain isocurvature modes Large scale B-mode polarization from primordial gravitational waves: - energy scale of inflation - rule out most ekpyrotic and pure curvaton/ inhomogeneous reheating models and others Small scale B-modes - Strong signal from any vector vorticity modes, strong magnetic fields, topological defects Weak lensing of CMB : - B-modes potentially confuse primordial signals - Important correction to theoretical linear result Foregrounds, systematics, etc, may make things much more complicated!

56 arXiv paper discussion and comments Also keyword-filtered listing of recent arXiv papers


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